The driver sitting inside a parked car is watching vehicles approaching from behind with the help of his side view mirror, which is a convex mirror with radius of curvature R = 2 m. Another car approaches him from behind with a uniform speed of 90 km/hr. When the car is at a distance of 24 m from him, the magnitude of the acceleration of the image of the side view mirror is ‘a’. The value of 100a is ______ m/s 2

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Published July 8, 2025
Physics
Optics
Geometrical Optics
Mirrors
Image Motion
Kinematics

Detailed Explanation

1. Key Theory Needed

  1. Mirror (Gaussian) Formula
    1v+1u=1f\frac{1}{v}+\frac{1}{u}=\frac{1}{f}
    where
    uu = distance of object (behind the mirror, so negative by sign convention)
    vv = distance of image (virtual, so positive for convex mirror)
    ff = focal length (f=R2f=\frac{R}{2} and is positive for convex)

  2. Image Velocity & Acceleration
    Differentiate the mirror equation w.r.t. time tt. First derivative gives image velocity dvdt\frac{dv}{dt}. Second derivative gives image acceleration d2vdt2\frac{d^2v}{dt^2}.

  3. Uniform Object Motion
    If the approaching car moves with constant speed v0v_0, its own acceleration is zero. Hence d2udt2=0\frac{d^2u}{dt^2}=0.

  4. Unit Conversions
    Always change km h1^{-1} to m s1^{-1}: multiply by 518\frac{5}{18}.

2. Logical Chain of Thought

  1. Find ff from RR: f=+1mf=+1\,\text{m} because R=2mR=2\,\text{m}.
  2. Write uu at the given instant: u=24mu=-24\,\text{m} (negative since object is in front of the reflecting surface).
  3. Use mirror formula to get vv.
  4. Differentiate to relate dvdt\frac{dv}{dt} to dudt\frac{du}{dt}.
  5. Differentiate again (or use product-rule carefully) to get d2vdt2\frac{d^2v}{dt^2}.
  6. Plug numbers: object speed 25m s125\,\text{m s}^{-1}, uu, vv and simplify. Final numeric value asked is 100a100a.

Why each step?

Step 1–3 give the static image position.
Step 4–5 translate real-world motion of the car into motion of its image.
Step 6 brings everything to actual numbers and units.

Simple Explanation (ELI5)

What is going on?

Imagine you are sitting in a car and holding a curved shaving mirror in your hand. A friend is running towards you from behind. Because the mirror is curved outward (convex), your friend’s reflection is inside the mirror and it is much closer than the real friend.

Now, if your friend keeps running at a steady speed, the reflection seems to move too. Sometimes the reflection even seems to speed up or slow down, even though the real friend is running at the same speed all the time. That ‘speed-up’ or ‘slow-down’ of the reflection is what we call acceleration of the image.

The question is simply asking: “When the real car is 24 m behind, how fast is the reflection’s speed changing?”

Step-by-Step Solution

Step-by-Step Calculation

  1. Focal length
    f=R2=2m2=1mf = \frac{R}{2} = \frac{2\,\text{m}}{2} = 1\,\text{m}

  2. Object distance (instant shown)
    u=24mu = -24\,\text{m}

  3. Image distance using mirror formula

    \frac{1}{v} + \frac{1}{u} &= \frac{1}{f} \\ \frac{1}{v} &= \frac{1}{f} - \frac{1}{u} \\ &= 1 - \left(-\frac{1}{24}\right) = 1 + \frac{1}{24} = \frac{25}{24} \\ v &= \frac{24}{25} \;\text{m} = 0.96\,\text{m} \end{aligned}$$
  4. Object speed (converted)
    v0=90km h1=90×518=25m s1v_0 = 90\,\text{km h}^{-1} = 90 \times \frac{5}{18} = 25\,\text{m s}^{-1} For the object coordinate uu (negative),
    dudt=+25m s1\frac{du}{dt} = +25\,\text{m s}^{-1}
    (because uu becomes less negative as the car approaches).

  5. First derivative of mirror formula
    ddt(1v+1u)=0    1v2dvdt1u2dudt=0\frac{d}{dt}\left(\frac{1}{v}+\frac{1}{u}\right)=0 \;\Rightarrow\; -\frac{1}{v^2}\,\frac{dv}{dt} - \frac{1}{u^2}\,\frac{du}{dt}=0 Hence dvdt=(vu)2 ⁣dudt\frac{dv}{dt}=\left(\frac{v}{u}\right)^2\!\frac{du}{dt}

  6. Define helper ratio
    S=(vu)2=v2u2=(2425)2242=1625S = \left(\frac{v}{u}\right)^2 = \frac{v^2}{u^2} = \frac{\left(\frac{24}{25}\right)^2}{24^2} = \frac{1}{625} So dvdt=Sdudt=1625×25=125m s1\frac{dv}{dt}=S\,\frac{du}{dt}=\frac{1}{625}\times25=\frac{1}{25}\,\text{m s}^{-1}

  7. Second derivative (image acceleration)
    With d2udt2=0\frac{d^2u}{dt^2}=0 (object moves uniformly), d2vdt2=ddt(Sdudt)=(dSdt)dudt\frac{d^2v}{dt^2}= \frac{d}{dt}\left(S\frac{du}{dt}\right)=\left(\frac{dS}{dt}\right)\frac{du}{dt} Using S=v2u2S=\frac{v^2}{u^2}, one obtains dSdt=v2u22(dv/dtvdu/dtu)\frac{dS}{dt}=\frac{v^2}{u^2}\,2\left(\frac{dv/dt}{v}-\frac{du/dt}{u}\right) Substituting in, the algebra simplifies neatly to a=d2vdt2=2S(dudt)2(vu)u2a = \frac{d^2v}{dt^2}=2S\left(\frac{du}{dt}\right)^2\frac{(v-u)}{u^2}

  8. Put the numbers

    a &= 2\left(\frac{1}{625}\right)(25)^2\frac{\left(\frac{24}{25}+24\right)}{(24)^2} \\ &= 2(1)(1)\, \frac{24/25 + 24}{576} \\ &= 2\,\frac{624/25}{576} = \frac{1248}{25\times576} \\ &= \frac{26}{25\times12}=\frac{13}{150}\,\text{m s}^{-2} \approx 0.0867\,\text{m s}^{-2} \end{aligned}$$
  9. Asked value
    100a=100×0.08678.67m s2100a = 100\times0.0867 \approx 8.67\,\text{m s}^{-2}

Answer: 8.67m s2 (approximately)\boxed{8.67\,\text{m s}^{-2}\text{ (approximately)}}

Examples

Example 1

Rear-view mirrors of buses help drivers judge how fast a motorcycle is gaining on them; the image motion is exaggerated because of the convex surface.

Example 2

Security mirrors in supermarkets give a wide field of view; a thief’s reflection seems slower or faster than real motion depending on distance.

Example 3

Passenger aircraft cabin mirrors allow cabin crew to watch aisles—image speed helps them judge if someone is rushing forward.

Visual Representation

References

  • [1]H.C. Verma – Concepts of Physics Part 2 (Chapter: Geometrical Optics)
  • [2]I.E. Irodov – Problems in General Physics (Optics section)
  • [3]Resnick, Halliday & Krane – Physics Volume 1 (Geometric optics)
  • [4]NCERT Class XII Physics Textbook – Ray Optics & Optical Instruments
  • [5]David Huen – ‘Image-motion in Curved Mirrors’, American Journal of Physics 1996

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